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8/18/2019 Aircraft Performance (lecture 1): Introduction
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AOE 3104 Lecture 1: Introduction
Andy Ko
Aerospace & Ocean Engineering DepartmentVirginia Polytechnic Institute & State University
*Most slides by C. A. Woolsey
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• Dimensions are qualitative, describing essential nature.
• In an MLT system, the four fundamental dimensions are:
Mass [M], Length [L], Time [T] , and Temperature [!]
• Other dimensions are derivable. Examples:
Force [F] = Mass [M] * Acceleration [L T-2]
= [M L T-2]
Speed [V] = Length [L] / Time [T]
= [L T-1]
Dimensions
3
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•
Units are quantitative, describing amount .
• Two common systems:
• US Customary Units
•
Système International d’Unités (SI Units)
Units
Dimension US Cust. Unit SI Unit
[M] slug kilogram (kg)
[L] foot (ft) meter (m)[T] second (s) second (s)
[!] ºR (ºF + 459.69) K (ºC + 273.16)
4Note: 1 slug = 14.5939 kg; 1 ft = 0.3048 m; 1 ºR = (1/1.8) K
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Units of Force
5
•
Units follow standard rules for mathematical composition.
• In an MLT system, the units of force are derived.
US Customary Units:
1 pound (lb or lbf ) = (1 slug)(1 ft/s2
)SI Units:
1 Newton (N) = (1 kg)(1 m/s2)
• These units are “proper” or “consistent.” No “magicconstants” are required to satisfy the physical law: F = m a.
Note: The value and units of a measurement are inseparable:
Length of a Ruler : 12 in = 30.48 cm = (1/660) furlongs
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Force vs. Mass mixup
•
Force and mass are not interchangeable – Mass is a measure of an object’s material
• Units: slugs, kilograms
– Force is the influence that tends to change the motion
of an object• Units: Pounds, Newton
• Pounds-force vs Pounds-mass
– 1 lbf = 1 slug * 1 ft/s2 = 1 lbm * 32.2 ft/s
2
–
So, 1 lbm weights 1 lbf on earth• lbf = 32.2 lbm-ft/s
2 = slug-ft/s2
– Confusing, isn’t it?
• Stick with lbs for force, and slugs for mass "
6
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Why pay attention to units?
•
Consistent frame of reference
•
Lessons from not paying attention to units
– Mar Climate Orbiter, September 1999, $125
million – Air Canada 143, Boeing 767, July 1983
•
Ran out of fuel in-flight
– Korean Air 6316, MD-11 freighter, April 1999
•
8 killed, 37 injured
7
A foolish man never learns from his mistakes. A goodman learns from his own mistakes, but a wise man
learns from the mistakes of others.
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Body & Inertial Frames
8Note: Attitude angles are not really measured about the body axes. More in AOE 3134...
Coordinate system is aligned with aircraftplane of symmetry
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Wind Frame
9
Angle of Attack:
Angle of Sideslip:
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Particle Representation
10
Newton’s 2nd Law of Motion:
Alternatively:
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The Forces
11
Newton’s 2nd Law of Motion:So what is F ?
• Externally generated fluid forces (aerostatic & aerodynamic)
•
Internally generated fluid forces (propulsion)• Gravitational forces
• Ground contact forces
Image: Albequerque Intl Balloon Fiesta
Aerostatic Forces Aerodynamic Forces
Image: NASA
Image: Boeing
Ground Contact ForcesPropulsion Forces
Image: Pratt & Whitney
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Aerostatic Force
12
Aerostatic force may be computed from Archimedes’ principle:
Image: Albequerque Intl Balloon Fiesta
Comments:• Most easily expressed in the inertial frame.
• Significant for “lighter-than-air (LTA)” vehicles.
Image: Goodyear
F aerostatic
=! ! gVol( ) z I
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Aerodynamic Force
13
The three components, resolved in the wind frame, are:
Drag:
Side Force:
Lift:
Comments:• Most easily expressed in the wind frame.
• Depends on fluid properties, vehicle geometry , andvehicle motion relative to the fluid.
! D x w
!SF yw
!
L z w
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Propulsion Force
14
Assume that propulsion acts in aircraft plane of symmetry:
Comments:
• Most easily expressed in the body frame.
•
Performance characteristics depend greatly on propulsion.
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Gravitational Force
15
Comments:
• Most easily expressed in the inertial frame.
•
Can change significantly over the course of a flight.
Image: USAF
The gravitational force is simply the vehicle’s weight:
F gravitational = m g( ) z I
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Ground Contact Force
16
Comments:
•
Most easily expressed in the inertial frame.
• Important for computing takeoff and landing distance.
Image: Boeing Image: USN
Neglecting cross-winds, ground contact force is:
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Types of Motion
•
Symmetric Motions: Motions in the inertial plane definedby the aircraft plane of symmetry, in wings level flight.
• Examples:
–
Wings-Level Cruise
– Wings-Level Climb/Descent
– Take-off & Landing
• Asymmetric Motions: “Out of symmetry plane” motions.
• Examples:
–
Banked turns –
Rolls
– Sideslipped landings
17
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Trajectory Equations
(Symmetric Flight)
18
Comments:
• To assess performance, must know how T, L, and D vary.
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Density
19
Definition: The density ( !) of a substance is the mass ofthat substance per unit volume.
Density is a scalar field. (It varies with location.)
Consider a differential volume element, with differential mass.
Assuming the fluid is a continuum:
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Temperature
20
Definition: Temperature is a measure of the averagemolecular kinetic energy.
Temperature is a scalar field.
High TemperatureLow Temperature
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Pressure
21
Definition: Pressure is the normal force exerted on asurface (physical or otherwise) per unit area.
Pressure is a scalar field.
Consider a differential area subject to a normal force.
Assuming the fluid is a continuum:
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Velocity
22
Definition: Fluid velocity is the rate of change of positionof an infinitesimally small fluid element at a point.
Velocity is a vector field.
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Fluid Flow Field
23
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Ideal Gas Law
24
Definition: An ideal gas is one for which intermolecularforces are negligible.
Equation of State for an Ideal Gas:
where R is the specific gas constant.
For air:
P = ! RT
R =!
M =
8314 J / kg !mole !K ( )28.96 kg / kg !mole( )
= 287.1 J
kg !K
=1716 ft ! lb
slug ! R
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Some Other Fluid Properties
25
Viscosity (µ): Ratio of shear stress to velocity gradient for aNewtonian fluid.
Specific Heat at Constant Pressure (cp): Ratio of heatadded to temperature increase, at constant pressure.
Specific Heat at Constant Volume (cv): Ratio of heat addedto temperature increase, at constant volume.
Ratio of Specific Heats*:
Speed of Sound:
Objective: Relate flow characteristics, including fluidproperties, to forces so we can assess performance.
*For air, the ratio of specific heats is 7/5 (or 1.4).
! = cP
/ cV
a = ! RT
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What next?
26
Hydrostatics and the Standard Atmosphere.
Week #2 Reading:
•
Anderson: Sections 2.1-4, 3.1-5, and 4.1-11• Optional: Watch Nova: Battle of the X-Planes
• http://www.hulu.com/watch/23356/nova-battle-of-the-x-planes
Homework : Will be posted today by 5pm